Optical sampling system for simultaneously monitoring intensity modulation and frequency modulation

ABSTRACT

The optical sampling system realizes the optical sampling by detecting the interference effect which is a linear correlation between the signal lights and the optical pulses, so that it suffices for both the signal lights and the optical pulses to have relatively low intensities, and the reception sensitivity is high. Also, the pulse width of the optical pulses and the amount of delay given to the optical pulses are the only factors that limit the time resolution, so that it is possible to provide the optical sampling system with excellent time resolution and power consumption properties, and it is possible for the optical sampling system to monitor not only the intensity of the signal lights but also the frequency modulation component as well.

BACKGROUND OF THE INVENTION

[0001] 1. Field of the Invention

[0002] The present invention relates to optical sampling method, system and program for monitoring repeatedly entered high speed signal lights, especially signal lights that are modulated at a speed that cannot be monitored by ordinary photo-detector element or electric circuit.

[0003] 2. Description of the Related Art

[0004] As a conventional optical sampling system, there has been a technique for monitoring low power and high speed repeating optical signals by monitoring linear correlation between signal lights and locally generated optical pulses, for example (see Japanese Patent Application Laid Open No. 9-162808 (1997), for example).

[0005] As shown in FIG. 2, in this conventional optical sampling system, the locally generated optical pulses from a sampling optical pulse generation unit 1 and the signal lights are injected into an optical hybrid 8, a plurality of output lights from this optical hybrid 8 are received by balanced optical receivers 5 a and 5 b, and output signals of these balanced optical receivers 5 a and 5 b are squared by square circuits 6 a and 6 b and then added together by an adder 7, so as to obtain an output proportional to an intensity of the signal lights at a time when the locally generated optical pulses and the signal lights overlap with each other. In this way, it is possible to realize an optical sampling operation with a time resolution equal to a pulse width of the locally generated optical pulses, without depending on a processing speed of electric circuits.

[0006] In general, the optical signals often receive he intensity modulation as well as the frequency modulation. For example, when the modulation by using the ON/OFF control of injection current of a semiconductor laser is applied, the intensity is of course changed, but at the same time the frequency of the generated laser beam is also changed. Also, in the case where the purely intensity modulated laser beam is transmitted through an optical fiber, the frequency of the optical signals after the transmission will receive the modulation due to the nonlinear optical effect of the optical fiber called self phase modulation.

[0007] Now, the conventional optical sampling system has been associated with the problem that the intensity change of the signal lights can be monitored but it cannot obtain any information regarding how the frequency has been changed.

BRIEF SUMMARY OF THE INVENTION

[0008] It is therefore an object of the present invention to provide optical sampling method, system and program capable of monitoring the intensity modulation information as well as the frequency modulation information of the signal lights simultaneously, while maintaining a high speed performance that can enable the monitoring of ultra high speed signal lights and a high sensitivity that can enable the monitoring of low power signal lights.

[0009] According to one aspect of the present invention there is provided an optical sampling method for monitoring repeatedly entered high speed signal lights, comprising the steps of: generating optical pulses with an optical pulse width shorter than an inverse of a frequency variation of the signal lights, which has a period slightly different from a repetition period of the signal lights, from an optical pulse generation unit; splitting each of the signal lights and the optical pulses into two parts by respective splitters; delaying a split part of either the signal lights or the optical pulses for a prescribed period of time by a delay unit; inputting one split parts of the signal lights and the optical pulses into a first optical hybrid, while inputting other split parts of the signal lights and the optical pulses into a second optical hybrid; receiving output lights from the first optical hybrid at first and second balanced optical receivers, and outputting first and second currents; receiving output lights from the second optical hybrid at third and fourth balanced optical receivers, and outputting this and fourth currents; and obtaining a frequency modulation component of the signal lights by carrying out a calculation processing with respect to values of the first to fourth currents by a calculation processing device.

[0010] According to another aspect of the present invention there is provided an optical sampling system for monitoring repeatedly entered high speed signal lights, comprising: an optical pulse generation unit configured to generate optical pulses with an optical pulse width shorter than an inverse of a frequency variation of the signal lights, which has a period slightly different from a repetition period of the signal lights; splitters configured to split each of the signal lights and the optical pulses into two parts; a delay unit configured to delay a split part of either the signal lights or the optical pulses for a prescribed period of time; a first optical hybrid configured to have one split parts of the signal lights and the optical pulses inputted therein; a second optical hybrid configured to have other split parts of the signal lights and the optical pulses inputted therein; first and second balanced optical receivers configured to receive output lights from the first optical hybrid, and output first and second currents; third and fourth balanced optical receivers configured to receive output lights from the second optical hybrid, and output this and fourth currents; and a calculation processing device configured to obtain a frequency modulation component of the signal lights by carrying out a calculation processing with respect to values of the first to fourth currents.

[0011] According to another aspect of the present invention there is provided a computer program product for causing a computer to function as a calculation processing device for obtaining a frequency modulation component of signal lights in an optical sampling system for monitoring repeatedly entered high speed signal lights, formed by: an optical pulse generation unit configured to generate optical pulses with an optical pulse width shorter than an inverse of a frequency variation of the signal lights, which has a period slightly different from a repetition period of the signal lights; splitters configured to split each of the signal lights and the optical pulses into two parts; a delay unit configured to delay a split part of either the signal lights or the optical pulses for a prescribed period of time; a first optical hybrid configured to have one split parts of the signal lights and the optical pulses inputted therein; a second optical hybrid configured to have other split parts of the signal lights and the optical pulses inputted therein; first and second balanced optical receivers configured to receive output lights from the first optical hybrid, and output first and second currents; third and fourth balanced optical receivers configured to receive output lights from the second optical hybrid, and output this and fourth currents; the computer program product comprising: a computer program code for causing the computer to obtain a frequency modulation component of the signal lights by carrying out a calculation processing with respect to values of the first to fourth currents.

[0012] Other features and advantages of the present invention will become apparent from the following description taken in conjunction with the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

[0013]FIG. 1 is a block diagram showing an exemplay configuration of an optical sampling system according to one embodiment of the present invention.

[0014]FIG. 2 is a block diagram showing an exemplary configuration of a conventional optical sampling system.

DETAILED DESCRIPTION OF THE INVENTION

[0015] Referring now to FIG. 1, one embodiment of an optical sampling system according to the present invention will be described in detail.

[0016]FIG. 1 shows an exemplary configuration of an optical sampling system according to one embodiment of the present invention. This optical sampling system is capable of obtaining not only the intensity but also the frequency modulation component of the signal lights that are repeatedly entered at a period of 1/f, and has a sine wave generator 2 for outputting sine wave electric signals of a period 1/(f+Δf) which is slightly different from the repetition period 1/f of the signal lights (Δf can be f/100 or f/1000, for example), and a sampling optical pulse generation unit 1 driven by the sine wave electric signals outputted from the sine wave generator 2, for generating sampling otical pulses with a period 1/(f+Δf) in which an offset Δf is added to the repetition period 1/f of the signal lights.

[0017] The sampling optical pulses that are locally generated optical pulses outputted from this sampling optical pulse generation unit 1 are split into two by a first splitter 11 a, and one of the splitted beams is entered into an optical coupler 4 a of a first optical 90° hybrid 8 a while the other one of the splitted beams is entered into an optical coupler 4 e of a second optical 90° hybrid 8 b after being delayed for a prescribed period of time by a delay unit 3. Also, the signal lights that are repeatedly entered at a period of 1/f are split into two by a second splitter 11 b, and one of the splitted beams is entered into an optical coupler 4 b of the first optical 90° hybrid 8 a while the other one of the splitted beams is entered into an optical coupler 4 f of the second optical 90° hybrid 8 b. The splitters 11 a and 11 b are formed by optical couplers or half mirrors, more specifically.

[0018] Note that the delay unit 3 delays the sampling optical pulses from the sampling optical pulse generation unit 1 through the splitter 11 a, but its purpose is to control a relative delay between the signal lights and the sampling optical pulses from the sampling optical pulse generation unit 1, so that it is also possible to provide the delay unit 3 at an output of the splitter 11 b instead of providing the delay unit 3 at an output of the splitter 11 a so as to delay the signal lights for a prescribed period of time.

[0019] The first and second optical 90° hybrids 8 a and 8 b (which will be referred to simply as optical hybrids hereafter) are formed by optical couplers 4 a, 4 b, 4 c and 4 d, and optical couplers 4 e, 4 f, 4 g and 4 h, respectively, and set up such that an optical path length difference between an optical path length A and an optical path length C becomes larger or smaller than an optical path length difference between an optical path length B and an optical path length D by λ/4 (where λis a wavelength of light). It is well known that the optical hybrid 8 can be realized by a free space optical system using half mirrors or an integrated optical circuit, for example.

[0020] Four output lights from the first optical hybrid 8 a are received by first and second balanced optical receivers 5 a and 5 b. Two output currents from these first and second balanced optical receivers 5 a and 5 b are applied with the waveform equalization at first and second low pass filters 10 a and 10 b which are set to have a blocking frequency approximately equal to an inverse of a dividing interval T, converted into numerical values by first and second numerical value deriving units 9 a and 9 b, and entered into a calculation processing device 13.

[0021] Also, four output lights from the second optical hybrid 8 b are received by third and fourth balanced optical receivers 5 c and 5 d. Two output currents from these third and fourth balanced optical receivers 5 c and 5 d are applied with the waveform equalization at third and fourth low pass filters 10 c and 10 d which are similarly set to have a blocking frequency approximately equal to an inverse of a dividing interval T, converted into numerical values by third and fourth numerical value deriving units 9 c and 9 d, and entered into the calculation processing device 13.

[0022] The calculation processing device 13 obtains a frequency modulation of the signal lights by carrying out a calculation processing to be described below, with respect to four numerical value signals entered as described above, i.e., four current values produced by the first to fourth balanced optical receivers 5 a to 5 d.

[0023] Next, the operation of the optical sampling system of this embodiment having the above described configuration will be described. The sampling optical pulses which are locally generated optical pulses outputted from the sampling optical pulse generation unit 1 are required to satisfy the following conditions.

[0024] (Condition #1) An intensity of the signal lights does not change hardly within a time period of a pulse width of the locally generated optical pulses.

[0025] (Condition #2) A frequency of the signal lights does not change hardly within a time period of a pulse width of the locally generated optical pulses.

[0026] (Condition #3) A central frequency of the optical pulses nearly coincides with a central frequency of the signal lights.

[0027] The above described conditions #1 and #2 imply that there is a need to provide the optical pulses which are shorter than the time resolution required for the optical sampling system.

[0028] In the following, the fact that the amplitude of signals can be detected correctly by the optical sampling system of the present invention when the above described conditions are satisfied will be described.

[0029] First, the waveforms of the signal light and the sampling optical pulse can be expressed by the following equaltions (1) and (2).

Sig(t)=A(t)exp{j[ω ₀+ω_(M)(t)]t}(signal light)  (1)

Sam(t)=δ(t−τ)exp(jω ₀ t+φ) (sampling optical pulse)  (2)

[0030] Here, A(t) is an amplitude of the signal light, ω_(M)(t) is a frequency modulation component of the signal light, δ(t−τ) is a central position of the optical pulse. Also, φ is a relative phase difference between the sampling optical pulse and the signal light, which changes randomly when the signal light and the sampling optical pulse are generated from separate lasers.

[0031] Because of the condition #3, both of the central frequencies of the signal light and the sampling optical pulse can be set to ω₀. At this point, the currents I₁(τ) and I₂(τ) that flow through the first and second balanced optical receivers 5 a and 5 b respectively can be expressed by the following equations (3) and (4). $\begin{matrix} \begin{matrix} {{I_{1}(\tau)} = {{Avr}\left\lbrack {{{{Sig}(t)}{{Sam}^{\bullet}(t)}{\exp\left( {j\left( {{{\omega_{M}(t)}t} + \varphi} \right)} \right\}}} + {c_{\bullet}c_{\bullet}}} \right\rbrack}} \\ {= {{{Avr}\left\lbrack {{{A(t)}{\delta^{\bullet}\left( {t - \tau} \right)}\exp \left\{ {j\left( {{{\omega_{M}(t)}t} + \varphi} \right)} \right\}} + {c_{\bullet}c_{\bullet}}} \right\rbrack}\quad \left( {{balanced}{\quad \quad}{optical}{\quad \quad}{receiver}\quad 5a} \right)}} \end{matrix} & (3) \\ \begin{matrix} {{I_{2}(\tau)} = {{Avr}\left\lbrack {{{{Sig}(t)}{{Sam}^{\bullet}(t)}\exp \left\{ {j\left( {{\pi \text{/}2} + {{\omega_{M}(t)}t} + \varphi} \right)} \right\}} + {c_{\bullet}c_{\bullet}}} \right\rbrack}} \\ {= {{{Avr}\left\lbrack {{{A(t)}{\delta^{\bullet}\left( {t - \tau} \right)}\exp \left\{ {j\left( {{\pi \text{/}2} + {{\omega_{M}(t)}t} + \varphi} \right)} \right\}} + {c_{\bullet}c_{\bullet}}} \right\rbrack}\left( {{balanced}{\quad \quad}{optical}\quad {receiver}\quad 5b} \right)}} \end{matrix} & (4) \end{matrix}$

[0032] Here, Avr indicates an average over about an integration time by the low pass filter 10 around a time τ. Also, δ(t) is a waveform of the locally generated pulse, which has finite values only around a time τ and which is zero elsewhere.

[0033] Also, because of the conditions #1 and #2, the intensity A(t) and the frequency φ_(M)(t) of the signal light do not change during the pulse width of δ(t) and their values are A(τ) and φ(τ), so that the currents I₁(τ) and I₂(τ) that flow through the first and second balanced optical receivers 5 a and 5 b respectively can be expressed by the following equations (5) and (6). $\begin{matrix} \begin{matrix} {{I_{1}(\tau)} = {{{\delta (0)}{A(\tau)}\exp \left\{ {j\left( {{{\omega_{M}(\tau)}\tau} + \varphi} \right)} \right\}} + {c_{\bullet}c_{\bullet}}}} \\ {= {{\delta (0)}{A(\tau)}{\cos \left( {{{\omega_{M}(\tau)}\tau} + \varphi} \right)}\left( {{balanced}\quad {optical}\quad {receiver}\quad 5a} \right)}} \end{matrix} & (5) \\ \begin{matrix} {{i_{2}(\tau)} = {{{A(\tau)}{\delta^{\bullet}(\tau)}\exp \left\{ {j\left( {{{\omega_{M}(\tau)}\tau} + \varphi + {\pi \text{/}2}} \right)} \right\}} + {c_{\bullet}c_{\bullet}}}} \\ {= {{\delta (0)}{A(\tau)}{\sin \left( {{{\omega_{M}(\tau)}\tau} + \varphi} \right)}\left( {{balanced}\quad {optical}\quad {receiver}\quad 5b} \right)}} \end{matrix} & (6) \end{matrix}$

[0034] Next, the currents I₃(τ) and I₄(τ) that flow through the third and fourth balanced optical receivers 5 c and 5 d respectively will be considered. The currents I₃(τ) and I₄(τ) that flow through the third and fourth balanced optical receivers 5 c and 5 d are basically the same as the currents I₁(τ) and I₂(τ) that flow through the first and second balanced optical receivers 5 a and 5 b, except that the delay unit 3 is inserted on a path of the sampling optical pulses which are the locally generated optical pulses from the sampling optical pulse generation unit 1.

[0035] When the path length difference due to the delay unit 3 is L, the signal lights and the locally generated optical pulses will enter the second optical hybrid 8 b with a time difference T given by the following equation (7).

T=L/c (where c is the speed of light)  (7)

[0036] There is a need to measure this path length difference L in advance, and it is necesary to maintain the wavelength level of the lights stably without any variation during the measurement.

[0037] In order to raise the time resolution of the optical sampling system of this embodiment to the maximum level, the time difference T=L/c should be set to the same level or within several times of the pulse width of the locally generated optical pulses. Namely, as will be described below, there is a need for the frequency of the signal lights to remain unchanged during the time difference T in order for the optical sampling system of this embodiment to operate properly.

[0038] The currents I₃(τ) and I₄(τ) that flow through the third and fourth balanced optical receivers 5 c and 5 d respectively can be expressed by the following equations (8) and (9). $\begin{matrix} \begin{matrix} {{I_{2}(\tau)} = {{Avr}\left\lbrack {{{{Sig}(t)}{{Sam}^{\bullet}\left( {t - T} \right)}\exp \left\{ {j\left( {{{\omega_{M}(t)}t} + \varphi} \right)} \right\}} + {c_{\bullet}c_{\bullet}}} \right\rbrack}} \\ {= {{{Avr}\left\lbrack {{{A(t)}{\delta^{\bullet}\left( {t - \left( {\tau + T} \right)} \right)}\exp \left\{ {j\left( {{{\omega_{M}(t)}t} + \varphi} \right)} \right\}} + {c_{\bullet}c_{\bullet}}} \right\rbrack}\left( {{balanced}{\quad \quad}{optional}\quad {receiver}\quad 5c} \right)}} \end{matrix} & (8) \\ \begin{matrix} {{I_{4}(\tau)} = {{Avr}\left\lbrack {{{{Sig}(t)}{{Sam}^{\bullet}\left( {t - T} \right)}\exp \left\{ {j\left( {{\pi \text{/}2} + {{\omega_{M}(t)}t} + \varphi} \right)} \right\}} + {c_{\bullet}c_{\bullet}}} \right\rbrack}} \\ {= {{{Avr}\left\lbrack {{{A(t)}{\delta^{\bullet}\left( {t - \left( {\tau - T} \right)} \right)}\exp \left\{ {j\left( {{\pi \text{/}2} + {{\omega_{M}(t)}t} + \varphi} \right)} \right\}} + {c_{\bullet}c_{\bullet}}} \right\rbrack}\left( {{balanced}\quad {optical}\quad {receicer}\quad 5d} \right)}} \end{matrix} & (9) \end{matrix}$

[0039] Then, by the calculation similar to those of the currents I₁(τ) and I₂(τ) described above, the currents I₃(τ) and I₄(τ) can be expressed by the following equations (10) and (11). $\begin{matrix} \begin{matrix} {{I_{2}(\tau)} = {{{A\left( {\tau + T} \right)}{\delta^{\bullet}(0)}\exp \left\{ {j\left( {{{\omega_{M}\left( {\tau + T} \right)}\left( {\tau + T} \right)} + \varphi} \right)} \right\}} + {c_{\bullet}c_{\bullet}}}} \\ {= {{\delta (0)}{A\left( {\tau + T} \right)}{\cos \left( {{{\omega_{M}\left( {\tau + T} \right)}\left( {\tau + T} \right)} + \varphi} \right)}\left( {{balanced}\quad {optical}\quad {receiver}\quad 5c} \right)}} \end{matrix} & (10) \\ \begin{matrix} {{I_{4}(\tau)} = {{{A(\tau)}{\delta^{\bullet}(0)}\exp \left\{ {j\left( {{{\omega_{M}\left( {\tau + T} \right)}\left( {\tau + T} \right)} + \varphi + {\pi \text{/}2}} \right)} \right\}} + {c_{\bullet}c_{\bullet}}}} \\ {{= {{\delta^{\bullet}(0)}{A\left( {\tau + T} \right)}{\sin \left( {{{\omega_{M}\left( {\tau + T} \right)}\left( {\tau + T} \right)} + \varphi} \right)}\left( {{balanced}\quad {optical}{\quad \quad}{receiver}\quad 5d} \right)}}\quad} \end{matrix} & (11) \end{matrix}$

[0040] As described above, in order to raise the time resolution of the optical sampling system of this embodiment to the maximum level, the time difference T=L/c is set to the same level or within several times of the pulse width of the locally generated optical pulses, and under this condition, the frequency ω_(M) of the signal lights does not change during the time difference T, so that the currents I₃(τ) and I₄(τ) can be expressed by the following equations (12) and (13). $\begin{matrix} {{{I_{2}(\tau)} = {{\delta^{\bullet}(0)}{A\left( {\tau + T} \right)}{\sin \left( {{{\omega_{M}\left( {\tau + T} \right)}\left( {\tau + T} \right)} + \varphi} \right)}\left( {{balance}\quad d\quad {optical}\quad {receiver}\quad 5c} \right)}}\quad} & (12) \\ {I_{4} = {(\tau){\delta^{\bullet}(0)}{A\left( {\tau + T} \right)}{\sin \left( {{{\omega_{M}(\tau)}\left( {\tau + T} \right)} + \varphi} \right)}\left( {{balanced}\quad {optical}\quad {receiver}\quad 5d} \right)}} & (13) \end{matrix}$

[0041] The currents I₁(τ), I₂(τ), I₃(τ) and I₄(τ) calculated as in the above are outputted from the first to fourth balanced optical receivers 5 a, 5 b, 5 c and 5 d, respectively, low pass filtered by the first to fourth low pass filters 10 a to 10 d, converted into numerical values by the first to fourth numerical value deriving units 9 a to 9 d, and supplied to the calculation processing device 13.

[0042] The calculation processing device 13 carries out the calculation for obtaining the frequency ω_(M)(τ) at a time τ of the signal lights from the equations (5), (6), (12) and (13) as follows.

[0043] First, the equation (6) is divided by the equation (5) and the equation (13) is divided by the equation (12) to obtain the following equations (14) and (15).

I ₂(τ)/I ₁(τ)=tan(ω_(M)(τ)τ+φ)  (14)

I ₄(τ)/I ₂(τ)=tan(ω_(M)(τ)(τ+T)+φ)  (15)

[0044] Consequently, the frequency ω_(M)(τ) can be calculated by the following equation (16).

ω_(M)(τ)={arctan(I ₄(τ)/I ₂(τ))−arctan(I ₂(τ)/I ₁(τ))}/T  (16)

[0045] By carrying out the calculation shown in the equation (16) at the calculation processing device 13 with respect to the output currents I₁(τ), I₂(τ), I₃(τ) and I₄(τ) of the balanced optical receivers 5 a to 5 d monitored as described above, it is possible to obtain the frequency modulation at a time τ of the signal lights.

[0046] Note that, from the output currents of the either pair of the balanced optical receivers 5, such as the currents I₁(τ) and I₂(τ), for example, it is of course also possible to obtain the intensity modulation component A(t) by carrying out the calculation of the following equation (17).

(I ₁(τ))²+(I ₂(τ))² ∝A ²(τ)  (17)

[0047] As described above, the optical sampling system of this embodiment realizes the optical sampling by detecting the interference effect which is a linear correlation between the signal lights and the optical pulses, so that it suffices for both the signal lights and the optical pulses to have relatively low intensities, and the reception sensitivity is high. Also, the pulse width of the optical pulses and the amount of delay given to the optical pulses are the only factors that limit the time resolution, so that it is possible to provide the optical sampling system with excellent time resolution and power consumption properties just as in the prior art, and while maintaining these properties, it is possible for the optical sampling system of this embodiment to monitor not only the intensity of the signal lights but also the frequency modulation component as well. As a result, it becomes possible to realize the optical sampling with a wider range of applications such as the monitoring of the frequency modulated or phase modulated lights that are used in the coherent optical transmission, for example, and the monitoring of the frequency modulation due to the self phase modulation at a time of the propagation inside the optical fiber.

[0048] Note that the calculation processing at the calculation processing device 13 of the optical sampling system of the above described embodiment should preferably be realized by a program.

[0049] As described above, according to the present invention, the optical pulses which have a period that is slightly different from the repetition period of the signal lights and a pulse width that is shorter than an inverse of a frequency variation of the signal lights are generated, the signal lights and the optical pulses are split, the one split parts of optical pulses and signal lights are entered into the first optical hybrid, other split parts of the signal lights and the optical pulses one of which is delayed after the splitting while the other one is not delayed are entered into the second optical hybrid, the output lights from the first and second optical hybrids are received by the first to fourth balanced optical receivers which output the first to fourth currents, and the frequency modulation component of the signal lights is obtained by the calculation processing of these first to fourth current values, so that it is possible to realize the optical sampling by detecting the interference effect which is a linear correlation between the signal lights and the optical pulses, it suffices for both the signal lights and the optical pulses to have relatively low intensities, the reception sensitivity is high, the time resolution and power consumption properties are excellent, and it is possible to monitor not only the intensity of the signal lights but also the frequency modulation component as well.

[0050] It is to be noted that the calculation processing device of the above described embodiments according to the present invention may be conveniently implemented using a conventional general purpose digital computer programmed according to the teachings of the present specification, as will be apparent to those skilled in the computer art. Appropriate software coding can readily be prepared by skilled programmers based on the teachings of the present disclosure, as will be apparent to those skilled in the software art.

[0051] In particular, the calculation processing device of the above described embodiments can be conveniently implemented in a form of a software package.

[0052] Such a software package can be a computer program product which employs a storage medium including stored computer code which is used to program a computer to perform the disclosed function and process of the present invention. The storage medium may include, but is not limited to, any type of conventional floppy disks, optical disks, CD-ROMs, magneto-optical disks, ROMs, RAMs, EPROMs, EEPROMs, magnetic or optical cards, or any other suitable media for storing electronic instructions.

[0053] It is also to be noted that, besides those already mentioned above, many modifications and variations of the above embodiments may be made without departing from the novel and advantageous features of the present invention.

[0054] Accordingly, all such modifications and variations are intended to be included within the scope of the appended claims. 

What is claimed is:
 1. An optical sampling method for monitoring repeatedly entered high speed signal lights, comprising the steps of: generating optical pulses with an optical pulse width shorter than an inverse of a frequency variation of the signal lights, which has a period slightly different from a repetition period of the signal lights, from an optical pulse generation unit; splitting each of the signal lights and the optical pulses into two parts by respective splitters; delaying a split part of either the signal lights or the optical pulses for a prescribed period of time by a delay unit; inputting one split parts of the signal lights and the optical pulses into a first optical hybrid, while inputting other split parts of the signal lights and the optical pulses into a second optical hybrid; receiving output lights from the first optical hybrid at first and second balanced optical receivers, and outputting first and second currents; receiving output lights from the second optical hybrid at third and fourth balanced optical receivers, and outputting this and fourth currents; and obtaining a frequency modulation component of the signal lights by carrying out a calculation processing with respect to values of the first to fourth currents by a calculation processing device.
 2. The optical sampling method of claim 1, wherein at the obtaining step, the calculation processing device carries out the calculation processing such that the first to fourth currents are applied with a waveform equalization by being low pass filtered through first to fourth low pass filter, converting first to fourth output currents of the first to fourth low pass filters into numerical values by a numerical value deriving units, and the calculation processing is carried out by using first to fourth current values obtained by the numerical value deriving units.
 3. The optical sampling method of claim 1, wherein at the obtaining step, when the first to fourth output currents from the first to fourth balanced optical receivers are I₁(τ), I₂(τ), I₃(τ) and I₄(τ), the calculation processing device carries out the calculation processing in which the second output current I₂(τ) is divided by the first output current I₁(τ), the fourth output current I₄(τ) is divided by the third output current I₂(τ), and the frequency modulation component of the signal lights is calculated according to two divided values, under a first condition that an intensity of the signal lights hardly changes during a time period of the optical pulse width of the optical pulses, a second condition that a frequency of the signal lights hardly changes during a time period of the optical pulse width of the optical pulses, and a third condition that a central frequency of the optical pulses nearly coincides with a central frequency of the signal lights.
 4. The optical sampling method of claim 3, wherein at the obtaining step, the calculation processing device calculates the frequency modulation component ω_(M)(τ) at a time τ by: ω_(M)(τ)={arctan(I ₄(τ)/I ₃(τ))−arctan(I ₂(τ)/I ₁(τ))}/T where T is a time difference given by the delay unit.
 5. An optical sampling system for monitoring repeatedly entered high speed signal lights, comprising: an optical pulse generation unit configured to generate optical pulses with an optical pulse width shorter than an inverse of a frequency variation of the signal lights, which has a period slightly different from a repetition period of the signal lights; splitters configured to split each of the signal lights and the optical pulses into two parts; a delay unit configured to delay a split part of either the signal lights or the optical pulses for a prescribed period of time; a first optical hybrid configured to have one split parts of the signal lights and the optical pulses inputted therein; a second optical hybrid configured to have other split parts of the signal lights and the optical pulses inputted therein; first and second balanced optical receivers configured to receive output lights from the first optical hybrid, and output first and second currents; third and fourth balanced optical receivers configured to receive output lights from the second optical hybrid, and output this and fourth currents; and a calculation processing device configured to obtain a frequency modulation component of the signal lights by carrying out a calculation processing with respect to values of the first to fourth currents.
 6. The optical sampling system of claim 5, wherein the calculation processing device carries out the calculation processing such that the first to fourth currents are applied with a waveform equalization by being low pass filtered through first to fourth low pass filter, converting first to fourth output currents of the first to fourth low pass filters into numerical values by a numerical value deriving units, and the calculation processing is carried out by using first to fourth current values obtained by the numerical value deriving units.
 7. The optical sampling system of claim 5, wherein when the first to fourth output currents from the first to fourth balanced optical receivers are I₁(τ), I₂(τ), I₃(τ) and I₄(τ), the calculation processing device carries out the calculation processing in which the second output current I₂(τ) is divided by the first output current I₁(τ), the fourth output current I₄(τ) is divided by the third output current I₃(τ), and the frequency modulation component of the signal lights is calculated according to two divided values, under a first condition that an intensity of the signal lights hardly changes during a time period of the optical pulse width of the optical pulses, a second condition that a frequency of the signal lights hardly changes during a time period of the optical pulse width of the optical pulses, and a third condition that a central frequency of the optical pulses nearly coincides with a central frequency of the signal lights.
 8. The optical sampling system of claim 7, wherein the calculation processing device calculates the frequency modulation component ω_(M)(τ) at a time τ by: ω_(M)(τ)={arctan(I ₄(τ)/I ₃(τ))−arctan(I ₂(τ)/I ₁(τ))}/T where T is a time difference given by the delay unit.
 9. A computer program product for causing a computer to function as a calculation processing device for obtaining a frequency modulation component of signal lights in an optical sampling system for monitoring repeatedly entered high speed signal lights, formed by: an optical pulse generation unit configured to generate optical pulses with an optical pulse width shorter than an inverse of a frequency variation of the signal lights, which has a period slightly different from a repetition period of the signal lights; splitters configured to split each of the signal lights and the optical pulses into two parts; a delay unit configured to delay a split part of either the signal lights or the optical pulses for a prescribed period of time; a first optical hybrid configured to have one split parts of the signal lights and the optical pulses inputted therein; a second optical hybrid configured to have other split parts of the signal lights and the optical pulses inputted therein; first and second balanced optical receivers configured to receive output lights from the first optical hybrid, and output first and second currents; third and fourth balanced optical receivers configured to receive output lights from the second optical hybrid, and output this and fourth currents; the computer program product comprising: a computer program code for causing the computer to obtain a frequency modulation component of the signal lights by carrying out a calculation processing with respect to values of the first to fourth currents.
 10. The computer program product of claim 9, wherein the computer program code causes the computer to carry out the calculation processing such that the first to fourth currents are applied with a waveform equalization by being low pass filtered through first to fourth low pass filter, converting first to fourth output currents of the first to fourth low pass filters into numerical values by a numerical value deriving units, and the calculation processing is carried out by using first to fourth current values obtained by the numerical value deriving units.
 11. The computer program product of claim 9, wherein when the first to fourth output currents from the first to fourth balanced optical receivers are I₁(τ), I₂(τ), I₃(τ) and I₄(τ), the computer program code causes the computer to carry out the calculation processing in which the second output current I₂(τ) is divided by the first output current I₁(τ), the fourth output current I₄(τ) is divided by the third output current I₃(τ), and the frequency modulation component of the signal lights is calculated according to two divided values, under a first condition that an intensity of the signal lights hardly changes during a time period of the optical pulse width of the optical pulses, a second condition that a frequency of the signal lights hardly changes during a time period of the optical pulse width of the optical pulses, and a third condition that a central frequency of the optical pulses nearly coincides with a central frequency of the signal lights.
 12. The computer program product of claim 11, wherein the computer program code causes the computer to calculate the frequency modulation component ω_(M)(τ) at a time τ by: ω_(M)(τ)={arctan(I ₄(τ)/I ₂(τ))−arctan(I ₂(τ)/I ₁(τ))}/T where T is a time difference given by the delay unit. 